Documents / Report

Defense Intelligence Reference Document Negative Mass Propulsion

Defense Intelligence Agency · 43 pages · text from the file's own layer

This Defense Intelligence Reference Document from the Defense Intelligence Agency is dated 3 January 2011. It was produced under the Advanced Aerospace Weapon System Applications (AAWSA) Program as part of a series of advanced technology reports. The report asks whether negative mass exists and whether it could be used for propulsion. It concludes that one route might be an ultra-light form of matter that could have gathered at the Moon's center. Reaching it would take a tunnel dug with thermonuclear shape charges.

  • p. 7 …sign, the total energy and momentum of the combined system remains zero for all times, leaving…
  • p. 8 …of special relativity, being the expression of a Minkowskian space-time structure, there is an older…
  • p. 10 …With lxl = (1/r, where OJ= 2tr/T, with T the time of revolution, and r…
  • p. 11 …time before their fields propagating with the velocity of light would reach the earth. Adding the…
  • p. 16 …Even though its time-averaged velocity is always less than the velocity of light, this means…
  • p. 18 …0~ m· =12r ~6X1Q-13g, ( 45) larger by a factor 3.6x10 11 times the mass…
  • p. 22 …by saying that the zero-point vacuum energy "generates" the Minkowski space-time. 7. Dynamic Interpretation…
  • p. 23 …the rod is /, and if the rod rests in the distinguished reference system, the time needed…
  • p. 24 …c -v Slll-1// -VCOSlf/ (67) with the time t' for a to and fro signal…
  • p. 25 …If tR is the absolute reflection time of the light signal at clock B, one has…
  • p. 26 …using a rod to measure the distance and the time it takes a light signal in…
  • p. 34 …The time needed to bring back the universe to its original low entropy state, is the…
  • p. 37 …times more dense than water 16. Suppose that in the center of the moon the accumulation…
  • p. 38 …the heat diffusion equation given by (109) where Xis the heat diffusion coefficient, the diffusion time…
  • p. 39 UNCLASSIFIED/ ,'P81l 81'1'11!111it 1!1!11!! 811LY The time needed for the liquid…
  • p. 42 …This means that a small, continuous removal of the heat through the injection and circulation of…
UNCLASSIFIED//F811. 8FFll!l*L 1!1!11! t!IIU:!Y
1. Introduction
If we extend the law of gravity to negative masses, but hold onto the equivalence of
inertial and gravitational masses, we have to distinguish between the following four
cases, if a test particle is placed near a gravitational field producing mass (Table 1):
Table 1. Interactions
Case Gravitational field Mass of test Motion of test
producing mass particle particle
1 + + attraction
2 + - attraction
3 - + repulsion
4 - - repulsion
Under the principle of equivalence if a negative test mass particle would be placed in
the gravitational field of earth, it would not fall upwards, as happens in science-fiction
antigravity machines. A test particle, regardless of whether it has positive or negative
mass, would there always fall down. It would fall upwards only if placed in the field of a
large negative mass.
A somewhat different situation arises if both masses, the field producing mass and the
mass of the test particle, have the same absolute value but are permitted to have
different signs. There we have to distinguish between the cases shown in Figure 1.
Ca:;o
2 -0 ---(-) '
l---- ~ o 11 ~ cc<>l(H a t1on
3 O· () .
-·-----
4 --(-) 0·._L ____ -~-
Figure 1. Forces
2
UNCLASSIFIED/ /F81it 8FFIIIAL ~:!II!! 8HLV

Not linked to a story yet.

About this file

Report, from the dia collection. The PDF is mirrored here; the original link is under it. 43 pages are in the text index: search them above, or from the library's search.